1. The Field of the Invention
Embodiments of the present invention relate generally to electron emitters and their methods of assembly. More particularly, disclosed embodiments are directed to electron emitter assemblies suitable for thermionic emission of electrons for x-ray generation.
2. The Relevant Technology
The x-ray tube has become essential in medical diagnostic imaging, medical therapy, and various medical testing and material analysis industries. Such equipment is commonly employed in areas such as medical diagnostic examination, therapeutic radiology, semiconductor fabrication, and materials analysis.
An x-ray tube typically includes a vacuum enclosure that contains a cathode assembly and an anode assembly. The vacuum enclosure may be composed of metal such as copper, glass, ceramic, or a combination thereof, and is typically disposed within an outer housing. At least a portion of the outer housing may be covered with a shielding layer (composed of, for example, lead or a similar x-ray attenuating material) for preventing the escape of x-rays produced within the vacuum enclosure. In addition, a cooling medium, such as a dielectric oil or similar coolant, can be disposed in the volume existing between the outer housing and the vacuum enclosure in order to dissipate heat from the surface of the vacuum enclosure. Depending on the configuration, heat can be removed from the coolant by circulating it to an external heat exchanger via a pump and fluid conduits. The cathode assembly generally consists of a metallic cathode head assembly and a source of electrons highly energized for generating x-rays. The anode assembly, which is generally manufactured from a refractory metal such as tungsten, includes a target surface that is oriented to receive electrons emitted by the cathode assembly.
During operation of the x-ray tube, the cathode is charged with a heating current that causes electrons to “boil” off the electron source by the process of thermionic emission. An electric potential on the order of about 4 kV to over about 200 kV is applied between the cathode and the anode in order to accelerate electrons boiled off the electron source toward the target surface of the anode assembly. X-rays are generated when the highly accelerated electrons strike the target anode surface.
Most of the electrons that strike the anode dissipate their energy in the form of heat. Some electrons, however, interact with the atoms that make up the target and generate x-rays. The wavelength of the x-rays produced depends in large part on the type of material used to form the anode surface. X-rays are generally produced on the anode surface through two separate phenomena. In the first, the electrons that strike the anode surface carry sufficient energy to “excite” or eject electrons from the inner orbitals of the atoms that make up the target. When these excited electrons return to their ground state, they give up the excitation energy in the form of x-rays with a characteristic wavelength. In the second process, some of the electrons from the cathode interact with the atoms of the target element such that the electrons are decelerated around them. These decelerating interactions are converted into x-rays by conservation of momentum through a process called bremsstrahlung. Some of the x-rays that are produced by these processes ultimately exit the x-ray tube through a window of the x-ray tube, and interact with a patient, a material sample, or another object.
Generating a tightly collimated x-ray beam for diagnostic purposes can be achieved by maximizing both x-ray flux (i.e., the number of x-ray photons emitted per unit time) and the focusing of the electron stream on the anode surface in order to produce a tightly collimated x-ray beam. Diagnostic image quality is at least partially a function of the number of electrons that impinge upon the target surface of the target anode. In general, more electrons results in higher x-ray flux, which in turn results in x-ray images with higher contrast (i.e., higher quality). In addition to emitter efficiency, the quality of diagnostic images can additionally depend on the pattern, or focal spot, created by the emitted beam of electrons on the target surface of the target anode. In general, a smaller focal spot produces a more highly focused or collimated beam of x-rays, which in turn produces better quality x-ray images.
In conventional x-ray tube designs, it is often difficult to achieve an optimal electron beam emission, due to a number of design constraints and tradeoffs. For example, emitter assemblies that utilize a planar emitter structure are desirable because such emitters are more useful for shaping the electron beam and consequent focal spot on the anode. However, planar emitters, due to their structure, are difficult to mount within a device due to the extremely high temperatures needed for thermionic emission. Such temperatures often exceed the capability of materials used in the planar emitter, and also lead to relatively large thermal expansion of the emitter assembly. Such thermal expansion often results in relative high variability in the resulting focal spots, which decreases the optical precision and ratability of the x-ray tube.
In one example embodiment, an emitter assembly utilizing a planar emitter configuration is disclosed. The emitter assembly in this example utilizes a structure to “clamp” the emitter between heat resistant elements. In disclosed embodiments, the clamping can be accomplished near the edges of the emitter, where the temperature excursions are not so extreme. For example, in one disclosed approach, the compressive force is applied to ceramic elements which sandwich the emitter between them. The compressive force is applied to the ceramic (or similar material) clamping materials during assembly by a metal clamp, or other ceramic members, tensioned to maintain the clamping force through the expected temperature range of the device during operation.
The heat resistant elements might be configured as separate structures in the form, for example, of an elongate rod. Alternatively, the heat resistant elements might be provided by way of a coating applied to surfaces of the emitter itself. Different sizes and/or shapes might be utilized to achieve different thermal isolation properties, depending on the needs of a particular application.
In another embodiment, methods of assembling an electron emitter assembly are disclosed. In one disclosed example, a method of assembly includes providing a support mount within an evacuated enclosure of an x-ray tube. An electron emitter is secured to the support mount in a manner such that the emitter is thermally isolated from the support mount. For example, in one embodiment, the emitter is secured to the support mount by disposing at least two heat resistant elements along an outer surface of the electron emitter, and then applying a force to the heat resistant elements so as to retain the emitter to the support mount. This approach insures that there is substantial thermal isolation between the support mount and the emitter during operation of the x-ray tube.
Disclosed embodiments provide a number of advantages. For example, use of a low thermal conduction material to clamp the emitter along its edges reduces waste heat that is conducted to the surrounding support structure. Moreover, compressive clamping forces applied to such high temperature materials (such as ceramic or PBN) takes advantage of this type of material's compressive strength at high temperatures. In addition, the ability to apply a clamping force at a point that is somewhat thermally isolated from the heated portion of the emitter (e.g. along its edges) means that the heat resistant elements are exposed to lower temperatures, thereby allowing a wider range of materials to be used—including less exotic and/or less expensive materials, thereby allowing for a lower cost support structure. Further, the disclosed clamping structure maintains a uniform operating temperature along the edges of the emitter, thereby simplifying the thermal design of the emitter itself and allowing accurate and repeatable performance in use. This results in low variability in the resulting focal spots—a condition that allows precision design of the x-ray optics and ratability of the x-ray tube.
This Summary is provided to introduce a selection of concepts in a simplified form that are further described below in the detailed description. This Summary is not intended to identify key features or essential characteristics of the claimed subject matter, nor is it intended to be used as an aid in determining the scope of the claimed subject matter. Moreover, it is to be understood that both the foregoing general description and the following detailed description of the present invention are exemplary and explanatory and are intended to provide further explanation of the invention as claimed.
To further clarify the above and other advantages and features of the present invention, a more particular description of the invention will be rendered by reference to specific embodiments thereof which are illustrated in the appended drawings. It is appreciated that these drawings depict only typical embodiments of the invention and are therefore not to be considered limiting of its scope. The invention will be described and explained with additional specificity and detail through the use of the accompanying drawings in which:
Example embodiments of the present invention are directed to a thermionic electron emitter designed to emit a beam of electrons for generating x-rays. The electron emitter is fabricated from a refractive metal that emits or “boils off” electrons when heated by an electrical current. Electron emission is dependent on the amount of current flowing through the electron emitter and on the temperature of the electron emitter. During the tube operation, the electron emitter expands. Various configurations of heat resistant elements, in conjunction with clamps, are provided to secure the electron emitter in place as the electron emitter expands thermally during tube operation.
Reference is first made to
In greater detail, the cathode assembly 50 is responsible for supplying a stream of electrons for producing x-rays, as previously described. While other configurations could be used, in the illustrated example the cathode assembly 50 includes a support structure 54 that supports a cathode head 56, which in turn supports an electron emitter assembly, designated generally at 200 and discussed in further detail below. In the example of
As mentioned, the cathode head 56 includes an electron emitter assembly 200 as an electron source for the production of the electrons 62 during tube operation. As such, the electron emitter assembly 200 is appropriately connected to an electrical power source (not shown) to enable the production by the assembly of the high-energy electrons, generally designated at 62.
The illustrated anode assembly 100 includes an anode 106, and an anode support assembly 108. The anode 106 comprises a substrate 110, here composed of graphite, and a target surface 112 disposed thereon. The target surface 112, in one example embodiment, comprises tungsten or tungsten rhenium, although it will be appreciated that depending on the application, other “high” Z materials/alloys might be used. A predetermined portion of the target surface 112 is positioned such that the stream of electrons 62 emitted by the electron emitter 200 and passed through the shield aperture 58A impinge on the target surface so as to produce the x-rays 130 for emission from the evacuated enclosure 20 via an x-ray transmissive window 132.
The kinetic energy resulting from the impingement of electrons on the target surface also yields large quantities of heat. Excess heat can be removed by way of a number of approaches and techniques. For example, in the disclosed embodiment a coolant is circulated through designated areas of the anode assembly 100 and/or other regions of the tube. Again, the structure and configuration of the anode assembly can vary from what is described herein while still residing within the claims of the present invention.
In the illustrated example, the anode 106 is supported by the anode support assembly 108, which generally comprises a bearing assembly 118, and a support shaft 120. The support shaft 120 is fixedly attached to a portion of the evacuated enclosure 20 such that the anode 106 is rotatably disposed about the support shaft via the bearing assembly 118, thereby enabling the anode to rotate with respect to the support shaft. Again, it should be appreciated that embodiments of the present invention can be practiced with anode assemblies having configurations that differ from that described herein. Moreover, in still other tube implementations and applications, the anode may be stationary.
While the example x-ray tube 10 of
The x-ray tube 10 of
Attention is now directed to
Shown as an example in
In one example embodiment the dimensions of the electron emitter 204 shown in
The electron emitter assembly 200 further includes at least two electrical connection points. The electrical connection points are in electrical communication with a power source via leads 226 (shown in
In one embodiment, the electron emitter 204 may be made of thorium doped tungsten, which may further include a carbon dopant (i.e., the thoriated tungsten is carburized). Carburization of a thoriated tungsten electron emitter assembly is typically achieved by subjecting the completed electron emitter assembly to a heat treatment in a hydrocarbon atmosphere consisting of a hydrogen carrier gas and benzene, naphthalene acetylene, or xylene. When the electron emitter assembly is heated in the presence of the hydrocarbon to a temperature on the order of 2000° C., the hydrocarbon is decomposed at the hot filament surface to form tungsten carbide that diffuses into the tungsten. Inclusion of the carbon dopant significantly increases the useful lifespan of an electron emitter assembly fabricated from thoriated tungsten by reducing the rate of thorium evaporation from the thoriated tungsten. Additional details regarding altering the work function of filaments can be found in U.S. application Ser. No. 11/350,975, entitled “Improved Cathode Structures for X-Ray Tubes,” filed Feb. 8, 2006, which is incorporated herein by reference in its entirety (referred to herein as the '975 application). Note that in other embodiments, the electron emitter may be made of other materials that include low work function materials that are suitable for thermionic electron emission when heated. Such material may also exhibit the property of having low thermal mass.
While others may be used, additional configurations of suitable electron emitter structures are also disclosed in: U.S. patent application Ser. No. 11/942,656 entitled “FILAMENT ASSEMBLY HAVING REDUCED ELECTRON BEAM TIME CONSTANT” and filed Nov. 19, 2007 (referred to herein as the '656 application); and U.S. patent application Ser. No. __/___,___ entitled “THERMIONIC EMITTER DESIGNED TO PROVIDE UNIFORM LOADING AND THERMAL COMPENSATION” (Attorney docket number 14374.159) filed Sep. 25, 2008; the contents of each of which are incorporated herein by reference in their entirety.
In the illustrated example, a first edge 240 of the emitter 204 is disposed between the heat resistant elements 220A and 220B, and a second edge 242 of the emitter 204 is disposed between the heat resistant elements 222A and 222B. Here, the heat resistant elements 220A, 220B, 222A, and 222B are secured in place via the compressive pressure applied by affixing the clamp 202 onto the supporting mount 206, thereby holding the emitter 204 in place via the heat resistant elements. The metal clamp 202 may be affixed onto the support mount 206 via screws, bolts, rivets, or other suitable attachment means.
In the example embodiment, the clamping is accomplished along the longitudinal edges of the emitter 204 (edges 240 and 242), and positioned where temperature excursions are not as extreme during tube operation. Moreover, since the clamping is provided via compressive force imposed on the heat resistant elements and tensioned so as to maintain a clamping force through the expected temperature excursions of the device during operation, the position of the emitter 204 is not affected by thermal expansion, and thus the focus and integrity of the electron beam (and the resulting focal spot) is maintained to a high precision. This ultimately results in higher image quality.
One example of the heat resistant elements 220A, 220B, 222A, and 222B are shown in the perspective view of
In an alternative embodiment, the heat resistant elements may be formed by applying a coating to the surface of the electron emitter along the respective edges. In one embodiment, this coating is applied electrophoretically, and the clamp is then secured to apply the compressive force directly to the respective coatings, thereby securing the emitter in place. Such an approach might be used, for example, for applications requiring a fast cooling emitter. With this approach, the clamp 202 material and the support structure 206 material might be chosen so as to have very high thermal conduction properties. Such materials might include, for example, molybdenum, TZM or nickel. Further details for this embodiment can be found in the '656 application, incorporated herein by reference.
In alternative embodiments, the heat resistant elements may also be configured so as to not be positioned directly across from the opposing heat resistant element, but in a manner so as to be in offset longitudinal positions with respect to each other. This approach—offsetting the opposing heat resistant elements from one another—utilizes the emitter material as a spring to further absorb expansion movement. One such approach is shown and described further in connection with
The material chosen to comprise the heat resistant element is one that provides adequate thermal isolation. However, other characteristics might also be sought, including high temperature resistance (for example, greater than about 1000° C.), good compressive rate, or any combination of thereof. The heat resistance element may be made of materials that include, but are not limited to, fully stabilized zirconia, aluminum nitrate, malite, pyrolytic boron nitride (PBN), or other suitable materials, such as other ceramics.
While a number of materials might be used for the clamp 202 and the supporting mount 206, suitable characteristics of the material might include high temperature strength. In one example, both the clamp and the mount are comprised of a metal, such as molybdenum or TZM. Other suitable materials might include, but are not limited to: nickel, stainless steel.
As will be appreciated from the foregoing, the disclosed emitter assembly 200 provides a number of advantages. Although other emitter configurations might be used, the disclosed embodiment is suitable for use with a planar emitter, which provides optimal electron beam emission. In addition, the disclosed structure allows for the use of the planar emitter in extremely high operating temperatures, and yet minimizes negative effects that would otherwise result from thermal expansion. In particular, the clamping configuration of the emitter assembly, including the use of the heat resistant elements 220 and 222, largely negates the effect of thermal expansion of the emitter and surrounding structures, and thereby insures a stable emitter assembly throughout the operating temperatures, and better overall electron stream resolution and resulting focal spot. Other advantages will be recognized through practice of the invention, as it is defined by the accompanying claims.
It will be appreciated that while one particular example embodiment has been described, other configurations and embodiments could be utilized for the emitter assembly. For example,
As is further shown in the embodiment of
In the embodiment of
In the embodiment of
In summary, embodiments of the present invention provide a number of advantages over the prior art. Disclosed embodiments provide a unique approach for mounting an electron emitter—including planar emitters—within an emitter assembly such that positioning (and hence electron emission accuracy) is not adversely affected by extreme operating temperatures. For example, use of a low thermal conduction material to clamp the emitter along its edges reduces waste heat that is conducted to the support structure. Moreover, compressive clamping forces applied to such high temperature materials (such as ceramic or PBN) takes advantage of this type of material's compressive strength at high temperatures. In addition, the ability to apply a clamping force at a point that is somewhat thermally isolated from the heated portion of the emitter (e.g. along its edges) means that the heat resistant elements are exposed to lower temperatures, thereby allowing a wider range of materials to be used—including less exotic and/or less expensive materials, thereby allowing for a lower cost support structure. Further, the disclosed clamping structure maintains a uniform operating temperature along the edges of the emitter, thereby simplifying the thermal design of the emitter itself and allowing accurate and repeatable performance in use. This results in low variability in the resulting focal spots—a condition that allows precision design of the x-ray optics and ratability of the x-ray tube.
The present invention may be embodied in other specific forms without departing from its spirit or essential characteristics. The described embodiments are to be considered in all respects only as illustrative and not restrictive. The scope of the invention is, therefore, indicated by the appended claims rather than by the foregoing description. All changes which come within the meaning and range of equivalency of the claims are to be embraced within their scope.